PL2230 series high energy full DPSS mode-locked Nd:YAG lasers

The first commercial fully diode pumped high pulse energy mode-locked laser, producing 28 ps pulses with up to 25 mJ pulse energy at a 50 Hz pulse repetition rate.

PL2250 series high energy picosecond mode-locked Nd:YAG lasers

Featuring up to 100 mJ pulse energy and <30 picosecond (20 ps optional) pulse duration, PL2250 series  picosecond mode-locked Nd:YAG lasers set new standard in high pulse energy picosecond lasers. Innovative and cost effective design allows to improve laser reliability, while reducing running and maintenance costs.

PL2210 series diode pumped picosecond Nd:YAG lasers

Short pulse duration, high energy, up to 2 kHz repetition rate and excellent pulse-to-pulse stability makes PL2210 series diode pumped picosecond lasers the first choice for many applications, like material processing, laser spectroscopy, optical parametric generator pumping and other tasks.

PL11M series - high pulse repetition rate lasers

PL11M series picosecond diode pumped laser offers 1 W output power at 1064 nm. It features high 1 MHz repetition rate, short 10 ps pulse duration and excellent beam quality (M² < 1.5). Stable output parameters and rugged cost-effective design establishes  PL11M series lasers as an excellent choice for various spectroscopy applications.

High energy picosecond mode-locked Nd:YLF lasers PL3140 series

PL3140 series mode-locked picosecond Nd:YLF lasers have excellent output parameters, are reliable and still remain simple and convienent to use.  Pulse duration as short as 10 ps is achieved without any sacrifice on beam quality.

Picosecond high energy Nd:YAG lasers SL230 series

SL 200 series lasers are excellent solution for applications, where high energy picosecond pulses are needed. Not like conventional mode-locked lasers that typically use saturable nonlinear absorption or Kerr lensing to produce ultrafast pulses, the SL200 series lasers employ backward stimulated Brillouin scattering (SBS) in liquid for the same purpose.

Picosecond high energy Nd:YAG lasers SL330 series

SL 300 series laser is excellent solution for applications that require high energy picosecond pulses. Pulse compression during backwardstimulated Brillouin scattering (SBS), used in EKSPLA SL300 series lasers, is simple and cost effective way for generating picosecond pulses and has unique capability of producing pulses with tunable duration.  

High energy and narrow linewidth picosecond OPG PGX01 series

PGX01 series picosecond optical parametric generators (OPGs) feature high pulse energy and narrow linewidth. PGX01 series OPGs are an excellent choice for researchers who need picosecond tunable source from UV to mid IR. Due to the unique tunability range these devices are a very attractive and cost-efficient alternative to other tunable laser radiation sources.

kHz repetition rate picosecond OPG PGX03 series

PGX03 series OPGs are excellent choice for researchers who need picosecond tunable sources from UV to mid IR. Featuring 1 kHz repetition rate and due to the unique broad tunability range these devices are a very attractive and cost-efficient alternative to other tunable laser radiation sources.

Narrow linewidth picosecond OPG PGX11 series

PGx11 series optical parametric generators offer broad output wavelength tuning - from 210 nm to 16 000 nm with nearly Fourier-transform limited linewidth (2 cm-1 and 0.5 cm-1) and low divergence.

PT200 series picosecond tunable lasers

PT200 series lasers integrate picosecond optical parametric oscillator and picosecond DPSS pump laser into single compact housing. Picosecond tunable lasers feature 690-3400 nm tuning range, 5 ps pulse duration, nearly Fourier transform-limited linewidth and up to 88 Mhz repetition rate. Megahertz pulse repetition rate is optimal for using photon-counting detection technique in numerous nonlinear spectroscopy and microscopy applications.

Autocorrelators

AC series scanning autocorrelator

Autocorrelators of AC series are designed for measurement of pulse duration of ultrafast lasers using the non-collinear second harmonic generation technique. Standard AC series models are targeted to work with mode-locked or SBS‑compressed Nd:YAG, or Nd:YLF lasers at fundamental or second harmonic wavelength.